6533b825fe1ef96bd12832cd
RESEARCH PRODUCT
Numerical study of shock formation in the dispersionless Kadomtsev-Petviashvili equation and dispersive regularizations
Christian KleinKristelle Roidotsubject
Mathematics::Analysis of PDEsFOS: Physical sciencesKadomtsev–Petviashvili equation01 natural sciences010305 fluids & plasmasDispersionless equationMathematics - Analysis of PDEsSingularity0103 physical sciencesFOS: MathematicsMathematics - Numerical Analysis0101 mathematicsKorteweg–de Vries equationFourier seriesMathematicsMathematical physicsNonlinear Sciences - Exactly Solvable and Integrable Systems010102 general mathematicsMathematical analysisStatistical and Nonlinear PhysicsNumerical Analysis (math.NA)Condensed Matter PhysicsBurgers' equationNonlinear Sciences::Exactly Solvable and Integrable SystemsDissipative systemGravitational singularityExactly Solvable and Integrable Systems (nlin.SI)Analysis of PDEs (math.AP)description
The formation of singularities in solutions to the dispersionless Kadomtsev-Petviashvili (dKP) equation is studied numerically for different classes of initial data. The asymptotic behavior of the Fourier coefficients is used to quantitatively identify the critical time and location and the type of the singularity. The approach is first tested in detail in 1+1 dimensions for the known case of the Hopf equation, where it is shown that the break-up of the solution can be identified with prescribed accuracy. For dissipative regularizations of this shock formation as the Burgers' equation and for dispersive regularizations as the Korteweg-de Vries equation, the Fourier coefficients indicate as expected global regularity of the solutions. The Kadomtsev-Petviashvili (KP) equation can be seen as a dispersive regularization of the dKP equation. The behavior of KP solutions for small dispersion parameter $\epsilon\ll 1$ near a break-up of corresponding dKP solutions is studied. It is found that the difference between KP and dKP solutions for the same initial data at the critical point scales roughly as $\epsilon^{2/7}$ as for the Korteweg-de Vries equation.
| year | journal | country | edition | language |
|---|---|---|---|---|
| 2013-04-24 | Physica D |